Microscope objective lens

ABSTRACT

A microscope objective lens is disclosed that includes, in order from the object side, a first lens group having positive refractive power, a second lens group having positive refractive power that is movable along the optical axis, and a third lens group. The first lens group includes, in order from the object side, two meniscus lens components, each with its concave surface on the object side, and at least one positive lens component, and the third lens group has adjacent concave lens element surfaces that face each other and are in contact with air. Specified conditions may be satisfied, and one or more lens components in the first lens group and the second lens group may be movable.

This application claims the benefit of foreign priority under 35 U.S.C.§119 of JP 2007-021,643 filed Jan. 31, 2007, the disclosure of which ishereby incorporated by reference.

BACKGROUND OF THE INVENTION

At present, in cutting edge research fields, for the purpose ofidentification of vital functions or behavioral analysis/interaction ofproteins, various techniques have been developed to observe living cellsover a period from a few days to several weeks. As a microscopeobservation technique for observing lesions within living cells, wideuse has been made of a fluorescence observation technique. In thisfluorescence observation technique, after biological samples (e.g.,living cells) have been dyed using a fluorescent material such as aspecific fluorescent protein as a luminescent marker, excitation lightis irradiated onto the biological samples so that fluorescence isgenerated. The presence and locations of specific sites within thebiological samples, such as lesions, are then detected by observing thesample.

An objective lens of a biological microscope is generally configured toobserve an object under observation (i.e., a specimen) through a coverglass. It is assumed that the thickness of the cover glass is a constantstandard value, and the aberrations that are generated by the coverglass are designed to be favorably corrected by the objective lens.However, production flaws are inherent in making cover glasses. Further,depending upon the particular observation technique used, there areoccasions during which an object under observation is observed through aflat plate having surfaces that are roughly parallel, such as a coverglass or a petri dish, but with the thickness of the flat plate beingdifferent from the standard value for which the objective lens wasdesigned.

Consequently, when the thickness of a cover glass is different from thestandard value, when the thickness fluctuates due to manufacturingtolerances, or when a combination of these two conditions occurs, theaberrations generated by the cover glass will not be sufficientlycorrected by the objective lens, and thus the image qualitydeteriorates. More specifically, the higher the numerical aperture(hereinafter NA) of the objective lens of the microscope, the moreapparent the deterioration of image quality becomes.

Japanese Laid Open Patent Application H03-58492 and Japanese Publication3371934 disclose conventional microscope objective lenses whereinaberrations generated by a cover glass, that is arranged between theplane of an object under observation and the objective lens, arecorrected either for the cover glass being of a non-standard thicknessor for having a thickness that fluctuates due to manufacturingtolerances.

BRIEF SUMMARY OF THE INVENTION

The present invention relates to a microscope objective lens that has ahigh NA wherein it is possible to acquire with a high signal-to-noiseratio a weak luminescence signal, while also having a wide field of viewand the capability to correct for aberrations caused by the cover glasshaving a different thickness than a thickness value for which theobjective lens was designed.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will become more fully understood from thedetailed description given below and the accompanying drawings, whichare given by way of illustration only and thus are not limitative of thepresent invention, wherein:

FIG. 1 is a cross-sectional view showing a cover glass CG, as well asthe lens element and lens group configuration along an optical axis of amicroscope objective lens according to Embodiment 1 of the presentinvention;

FIGS. 2A-2D show the spherical aberration, astigmatism, lateral color,and distortion, respectively, of the microscope objective lens shown inFIG. 1;

FIG. 3 is a cross-sectional view showing a cover glass CG, as well asthe lens element and lens group configuration along an optical axis of amicroscope objective lens according to Embodiment 2 of the presentinvention;

FIGS. 4A-4D show the spherical aberration, astigmatism, lateral color,and distortion, respectively, of the microscope objective lens shown inFIG. 3; and

FIG. 5 is a cross-sectional view showing the lens element configurationalong an optical axis of an imaging lens that may be combined witheither of the microscope objective lenses shown in FIGS. 1 and 3.

DETAILED DESCRIPTION

In fluorescence observations, if some type of excitation (such asirradiation using an excitation light) is applied to a biologicalsample, there is a possibility that the excitation may adversely affectan activation state of the cells. Consequently there is high demand fora microscope system wherein a luminescent marker may be excited byusing, to the extent possible, an excitation light having a weakintensity, and wherein a weak luminescence signal, which is generated inresponse to the excitation, can be detected with an extremely highefficiency.

Further, there is also high demand for a microscope system wherein aloss of sight due to the movement of living cells out of the observationfield can be prevented by providing a microscope system that enablessimultaneously observing, over a wide field of view, information frommany cells that is detected at once. In addition, there is the usualdemand for high processing speed and improvements in operationalefficiency. However, no microscope device or system that is currentlyavailable satisfies these requirements.

The objective lenses described in Japanese Laid Open Patent ApplicationH03-58492 and in Japanese Patent Publication 3371934 are not suitablefor use in a microscope device or system that satisfies theserequirements. The applicant of the present application has previouslyproposed, in Japanese Patent Application No. 2005-188086, a microscopeobjective lens that does satisfy these requirements (i.e., one that hasa high NA, thus enabling the acquisition of a weak luminescence signalwith high signal-to-noise ratio S/N) as well as a microscope system thatis equipped with such a microscope objective lens. However, themicroscope objective lens disclosed in Japanese Patent Application No.2005-188086 does not provide for any way to correct for aberrationsassociated with a fluctuation in cover glass thickness due tomanufacturing tolerances or for using a different thickness of coverglass than that for which the microscope objective lens was designed.Further, in biological microscope observations, not only any change inthe cover glass thickness, but also any change in ambient temperature(e.g., using a microscope at elevated ambient temperatures to promotecell culturing) will cause a variation in aberrations. Thus, there is aneed to have the microscope objective lens disclosed in Japanese PatentApplication No. 2005-188086 be capable of correcting for a variation inaberrations caused by both cover glass thickness variations and ambienttemperature variations.

The object of the present invention is to provide a microscope objectivelens that has a high NA for enabling the acquisition of a weak signalwith a high S/N, while maintaining excellent correction of variousaberrations and providing a wide observation field of view such that themicroscope objective lens maintains compatibility with a conventionalmicroscope system.

The term “lens element” is herein defined as a single transparent massof refractive material having two opposed refracting surfaces, whichsurfaces are positioned at least generally transversely of the opticalaxis of the microscope objective lens. The term “lens component” isherein defined as (a) a single lens element spaced so far from anyadjacent lens element that the spacing cannot be neglected in computingthe optical image forming properties of the lens elements or (b) two ormore lens elements that have their adjacent lens surfaces either in fulloverall contact or overall so close together that the spacings betweenadjacent lens surfaces of the different lens elements are so small thatthe spacings can be neglected in computing the optical image formingproperties of the two or more lens elements. Thus, some lens elementsmay also be lens components. Therefore, the terms “lens element” and“lens component” should not be taken as mutually exclusive terms. Infact, the terms may frequently be used to describe a single lens elementin accordance with part (a) above of the definition of a “lenscomponent.”

The microscope objective lens of the present invention includes, inorder from the object side, a first lens group having positiverefractive power, a second lens group having positive refractive powerthat is movable along the optical axis (as shown by the double-headedarrow), and a third lens group. The first lens group includes, in orderfrom the object side, two meniscus lens components, each with itsconcave surface on the object side, and at least one positive lenscomponent, and the third lens group has adjacent concave lens elementsurfaces that face each other and are in contact with air.

Further, it is preferable that the microscope objective lens of thepresent invention satisfies the following conditions:

7≦f  Condition (1)

0.5<NA  Condition (2)

where

f is the focal length (in mm) of the objective lens, and

NA is the numerical aperture of the objective lens on its object side.

In the microscope objective lens of the present invention, it ispreferable that the movement of the second lens group be for correctionof aberrations associated with having a non-standard thickness of aroughly plane-parallel plate that may be positioned between an objectunder observation and the first lens group. The non-standard thicknessmay result from manufacturing tolerances or from using a plane-parallelplate of a uniform but non-standard thickness, or both.

Still further, in the microscope objective lens of the presentinvention, it is preferable that the second lens group satisfies thefollowing condition:

0.8≦|β2|≦1.2  Condition (3)

where

β2 is the lateral magnification of the second lens group when the objectof the second lens group is the image formed by the first lens group.

In the microscope objective lens of the present invention, it ispreferable that a positive lens component, which is located on the imageside of the two meniscus lens components in the first lens group, ismovable along the optical axis so as to enable aberrations caused by achange in ambient temperature of the objective lens to be corrected.

Moreover, it is preferable that the microscope objective lens of thepresent invention satisfies the following condition:

60<D≦120  Condition (4)

where

D is the on-axis distance (in mm) measured from the object underobservation to a mounting plane S, with the mounting plane S being aplane where the objective lens is mounted to a microscope body.

By requiring the first lens group to include two meniscus lenscomponents, each with a concave surface on the object side and arrangedsequentially along the optical axis, the ray height can be graduallyincreased without using excessive refractive power. By requiring thesecond lens group to have positive refractive power, the ray height doesnot have to increase more than is necessary, so the generation ofaberrations can be minimized. By requiring the third lens group to havetwo lens components with adjacent facing concave surfaces that contactair, the Petzval sum can be made small. Furthermore, from the point ofview of reducing the number of lens elements and simplifying the lenselement configuration, it is desirable that there be a single pair oflens components having adjacent facing concave surfaces that contactair.

By ensuring that Conditions (1) and (2) above are satisfied, anobjective lens may be provided that is suitable for use in themicroscope device and the microscope system disclosed in Japanese PatentApplication 2005-188086. Thus, an objective lens may be provided thathas a high NA and a broad field of view while maintaining compatibilitywith a conventional microscope system.

Further, in the microscope objective lens of the present invention,preferably the movement of the second lens group along the optical axisis for correction of aberration variations associated with anon-standard thickness of a roughly-parallel flat plate that may bearranged between an object under observation and the first lens group.With this configuration, an objective lens having a broad field of viewand a high NA that simultaneously enables correction of aberrationvariations associated with a non-standard thickness of aroughly-parallel flat plate that may be arranged between an object underobservation and the first lens group is provided.

When Condition (3) above is satisfied, even if the cover glass thicknessvaries, if a cover glass of a different thickness is used, or both, thefluctuation of the image point position can be controlled as much aspossible, and an objective lens having a broad field of view and a highNA wherein aberration corrections are improved can be provided.

In order to reduce a fluctuation of the image point position when thesecond lens group is moved, it is necessary to reduce the refractivepower of the second lens group. For example, if the second lens groupwere to be formed of only a plane-parallel glass plate, the image pointwould not move along the optical axis when the second lens group ismoved along the optical axis. In this case, the refractive power of thesecond lens group would be zero and the magnification of the second lensgroup for an object at infinity would be 1. If the second lens group forcorrecting the aberrations with respect to paraxial rays functionssubstantially the same as plane-parallel glass plates, the movement ofthe image point will be minimal. Therefore, for the purpose of reducingthe movement of the image point as much as possible when the second lensgroup is moved along the optical axis, it is necessary that therefractive power of the second lens group be reduced as much aspossible. Moreover, the magnification of the second lens group should benear unity.

If Condition (3) above is not satisfied, the movement of the image pointbecomes greater and adequately correcting the various aberrationsbecomes difficult.

Further, in the microscope objective lens of the present invention, itis preferable that a positive lens component in the first lens group,which is on the image side of the two meniscus lens components in thefirst lens group, is movable along the optical axis so as to enable thecorrection of aberration variations associated with a change intemperature of the microscope objective lens, as when the ambienttemperature is increased above normal room temperature to promote cellculturing.

If the lower limit of Condition (4) is not satisfied, there will beinsufficient space for providing a sufficient number of lens elements toadequately correct various aberrations. On the other hand, if the upperlimit value of Condition (4) is not satisfied, the overall size of theobjective lens will become too large, thereby making miniaturization ofthe overall microscope system difficult.

Two embodiments of the invention will now be described in detail withreference to the drawings.

Embodiment 1

FIG. 1 is a cross-sectional view showing the lens element and lens groupconfiguration along an optical axis of the microscope objective lensaccording to Embodiment 1 of the present invention. As shown in FIG. 1,the microscope objective lens of this embodiment is formed of, in orderfrom the object side, a first lens group G1, a second lens group G2, anda third lens group G3. In addition, on the left side of the microscopeobjective lens shown in FIG. 1 there is a cover glass CG.

The first lens group G1 is formed of, in order from the object side, afirst meniscus lens element L11 of positive refractive power with itsconcave surface on the object side, a second meniscus lens element L12with its concave surface on the object side, a plano-convex lens L13with its planar lens surface on the object side, and a cemented lenscomponent of positive refractive power that is formed of a biconvex lenselement L14 cemented to a biconcave lens element L15.

The second lens group G2 is formed of a plano-convex lens element L21with its planar surface on the object side. Furthermore, the second lensgroup G2 is configured to be movable along the optical axis so as toenable correction of aberration variations associated with a change inthickness of a roughly parallel flat plate, such as a cover glass CG ora petri dish, that is arranged between an object under observation andthe first lens group G1.

The third lens group G3 is formed of, in order from the object side, acemented lens component formed of a plano-concave lens element L31 withits concave surface on the image side cemented to a biconvex lenselement L32, a cemented lens component formed of a biconvex lens elementL33 cemented to a biconcave lens element L34, a cemented lens componentformed of a meniscus lens element L35 of negative refractive power withits convex surface on the image side cemented to a meniscus lens elementL36 of positive refractive power with its concave surface on the objectside, and yet another cemented lens component formed of a plano-concavelens element L37 with its planar surface on the image side cemented to aplano-convex lens element L38 with its planar surface on the objectside. A pair of adjacent facing concave surfaces that are in contactwith air are provided by the image-side surface of biconcave lenselement L34 and the object-side surface of meniscus lens element L35.

Table 1 below lists numerical data of the optical members that comprisethe microscope objective lens of Embodiment 1. In the top portion of thetable are listed the cover glass thickness (in mm), the focal length f(in mm), the numerical aperture NA, and the value of β2, where β2 is thelateral magnification of the second lens group when the object of thesecond lens group is the image formed by the first lens group. In themiddle portion of the table are listed, in order from the object side,the radius of curvature r_(i) (for i=1-23) of each lens element surface,the on-axis spacing between lens elements di (for i=1-22), the index ofrefraction nd (at the d-line wavelength of 587.6 nm) of each opticalelement to the right of a surface i, and the Abbe number νdi of eachoptical element to the right of a surface i. In the bottom portion ofthe table is listed the on-axis distance value (in mm) from the surfaceof r23 to the plane S (with S being a plane where the microscopeobjective lens is mounted to the microscope body, with the directionfrom the surface of r23 toward the object being indicated by a negativevalue), the value of d0 (in mm), where d0 is the on-axis distance fromthe cover glass CG to the first lens element surface of radius ofcurvature r1, as well as the values of d9, d11 and D for three differentthicknesses of cover glass, namely, 0.1204 mm, 0.17 mm, and 0.249 mm.

TABLE 1 Cover glass thickness: 0.17 mm f = 18 mm NA = 0.8 β2 = −1.11 r1= −7.3878 d1 = 7.7502 nd1 = 1.7865 νd1 = 50 r2 = −8.0452 d2 = 0.7875 r3= −8.8338 d3 = 6.1369 nd3 = 1.603 νd3 = 65.44 r4 = −11.3001 d4 = 0.4246r5 = ∞ d5 = 4.4184 nd5 = 1.497 νd5 = 81.54 r6 = −21.451 d6 = 0.1139 r7 =21.7103 d7 = 7.8237 nd7 = 1.43875 νd7 = 94.93 r8 = −28.7977 d8 = 2.4 nd8= 1.7725 νd8 = 49.6 r9 = 192.794 d9 = 1.9779 r10 = ∞ d10 = 2.9889 nd10 =1.43875 νd10 = 94.93 r11 = −32.0412 d11 = 0.4775 r12 = ∞ d12 = 2.3 nd12= 1.7725 νd12 = 49.6 r13 = 15.6187 d13 = 8.8294 nd13 = 1.43875 νd13 =94.93 r14 = −21.5268 d14 = 0.4918 r15 = 17.755 d15 = 6.337 nd15 =1.43875 νd15 = 94.93 r16 = −35.4936 d16 = 2.1 nd16 = 1.6134 νd16 = 44.27r17 = 15.8401 d17 = 8.7105 r18 = −10.6688 d18 = 2.4 nd18 = 1.788 νd18 =47.37 r19 = −28.6362 d19 = 6.8611 nd19 = 1.43875 νd19 = 94.93 r20 =−14.2704 d20 = 0.5298 r21 = −52.7292 d21 = 3.3 nd21 = 1.51633 νd21 =64.14 r22 = ∞ d22 = 5.5916 nd22 = 1.673 νd22 = 38.15 r23 = −30.4292On-axis distance from the surface of r23 to the plane S equals −10 mm

Cover glass thickness d0 d9 d11 D 0.1204 mm  1.2804 2.1412 0.314374.1516  0.17 mm 1.248 1.9779 0.4775 74.1687 0.249 mm 1.1965 1.70390.7516 74.1963

FIGS. 2A-2D show the spherical aberration (in mm), astigmatism (in mm),lateral color (in mm), and distortion (in %), respectively, of themicroscope objective lens of Embodiment 1. In FIG. 2A, the label “0.8”above the ordinate indicates the maximum NA. In FIG. 2B, the astigmatismis shown for both the sagittal image surface ΔS and meridional imagesurface ΔM. In FIG. 2A, the ordinate position of the maximum NA (NA=0.8)times 0.5 and times 0.7 is labeled. In FIGS. 2B-2D, the label “11.00”above the ordinate indicates the maximum image height (in mm). In FIGS.2B and 2D, the ordinate positions of the maximum image height (11.00 mm)times 0.5 and times 0.7 are shown. In FIG. 2C, the ordinate positions ofmaximum image height (11.00) times plus 0.941 and times minus 0.941 (asmeasured vertically from the optical axis) are labeled on the ordinate,and the abscissa is labeled at −2.00 mm and +2.00 mm of lateral color.In FIGS. 2A and 2C, curves are shown for the four wavelengths listed.

Embodiment 2

FIG. 3 is a cross-sectional view along the optical axis showing the lenselement and lens group configuration of the microscope objective lensaccording to Embodiment 2 of the present invention. As shown in FIG. 3,the microscope objective lens of Embodiment 2 is similar to that ofEmbodiment 1 in that the microscope objective lens of Embodiment 2 isalso formed of, in order from the object side, a first lens group G1, asecond lens group G2 and a third lens group G3. Once again, CG is thecover glass. This embodiment differs from that shown in FIG. 1 primarilyin that a positive lens element of the first lens group is movable alongthe optical axis, as shown by the double-headed arrow below lens elementL13′. In addition, most of the construction values, such as given inTable 1 for Embodiment 1, are different, as will be apparent from Table2.

The first lens group G1 is formed of a first positive meniscus lenselement L11 with its concave surface on the object side, a secondmeniscus single lens element L12 with its concave surface on the objectside, a biconvex lens element L13′, and a cemented lens component havingpositive refractive power overall formed of a biconvex lens element L14that is cemented to a biconcave lens element L15.

As mentioned above, the biconvex lens element L13′ is movable along theoptical axis so as to enable the correction of the aberration variationsassociated with a change in temperature of the microscope objectivelens.

The second lens group G2 is formed of a biconvex lens element L21′.Further, the second lens group G2 may be moved along the optical axis(as shown by the double-headed arrow) so as to enable the correction ofthe aberration variations associated with the thickness of aroughly-parallel flat plate CG, such as a cover glass or a petri dishthat may be arranged between an object under observation and the firstlens group G1, being a non-standard value (i.e., different than thethickness of a cover glass for which the microscope was designed).

The third lens group G3 is formed of, in order from the object side, acemented lens component formed of a biconcave lens element L31′ that iscemented to a biconvex lens element L32, another cemented lens componentformed of a biconvex lens element L33 that is cemented to a biconcavelens element L34, another cemented lens component formed of a negativemeniscus lens element L35 with its convex surface on the image sidecemented to a positive meniscus lens element L36 with its concavesurface on the object side, and another cemented lens component formedof a negative meniscus lens element L37′ with its convex surface on theimage side cemented to a positive meniscus lens element L38′ with itsconcave surface on the object side. A pair of adjacent concave surfacesthat are in contact with air are formed by facing surfaces of thebiconcave lens element L34 and the negative meniscus lens L35.

Table 2 below lists numerical data of the optical members that comprisethe microscope objective lens of Embodiment 2. In the top portion of thetable are listed the cover glass thickness (in mm) at room temperature,the focal length f (in mm), the numerical aperture NA, and the value ofβ2, where β2 is the lateral magnification of the second lens group whenthe object of the second lens group is the image formed by the firstlens group. In the middle portion of the table are listed, in order fromthe object side, the radius of curvature r_(i) (for i=1 to 23) of eachlens element surface, the on-axis spacing between lens elements di (fori=1 to 22), the index of refraction nd (at the d-line wavelength of587.6 nm) of each optical element to the right of a surface i, and theAbbe number νdi of each optical element to the right of a surface i. Inthe bottom portion of the table is listed the on-axis distance value (inmm) from the surface of r23 to the plane S (with S being a plane wherethe microscope objective lens is mounted to the microscope body, withthe direction from the surface of r23 toward the object being indicatedby a negative value), as well as the values (in mm) of d0, d4, d6, d9,d11 and D for three different thicknesses of cover glass (in mm) and twodifferent ambient temperatures, namely, 21° C. (room temperature) and37° C.

TABLE 2 Cover glass thickness: 0.1757 mm at room temperature (21° C.) f= 17.95 mm NA = 0.8 β2 = −1.07 r1 = −6.2893 d1 = 7.435 nd1 = 1.788 νd1 =47.37 r2 = −8.4983 d2 = 0.435 r3 = −10.1532 d3 = 6.314 nd3 = 1.603 νd3 =65.44 r4 = −11.3001 d4 = 0.1634 r5 = 123.3491 d5 = 5.3088 nd5 = 1.497νd5 = 81.54 r6 = −22.1261 d6 = 0.6147 r7 = 22.8619 d7 = 8.5103 nd7 =1.497 νd7 = 81.54 r8 = −23.4122 d8 = 2.5 nd8 = 1.7725 νd8 = 49.6 r9 =58.226 d9 = 1.2807 r10 = 177.3687 d10 = 4.016 nd10 = 1.497 νd10 = 81.54r11 = −26.1937 d11 = 0.4724 r12 = −154.047 d12 = 2.4 nd12 = 1.7725 νd12= 49.6 r13 = 15.83 d13 = 7.7124 nd13 = 1.43875 νd13 = 94.93 r14 =−22.5419 d14 = 0.1279 r15 = 16.67 d15 = 6.3026 nd15 = 1.43875 νd15 =94.93 r16 = −35.2899 d16 = 2.1 nd16 = 1.6134 νd16 = 44.27 r17 = 15.1661d17 = 9.4155 r18 = −10.7118 d18 = 2.503 nd18 = 1.788 νd18 = 47.37 r19 =−28.9605 d19 = 6.5584 nd19 = 1.43875 νd19 = 94.93 r20 = −14.3451 d20 =0.5248 r21 = −57.7601 d21 = 3.3962 nd21 = 1.51633 νd21 = 64.14 r22 =−486.9661 d22 = 5.4523 nd22 = 1.673 νd22 = 38.15 r23 = −29.6884On-axis distance from the surface of r23 to the mounting plane S equals−10 mm

Ambient Cover glass temperature Thickness d0 d4 d6 d9 d11 D 21° C.0.1235 1.3975 0.1634 0.6147 1.408 0.345 75.0643 21° C. 0.1757 1.36340.1634 0.6147 1.2807 0.4724 75.0825 21° C. 0.254 1.3124 0.1634 0.61471.0746 0.6784 75.1097 37° C. 0.1197 1.3883 0.672 0.12 1.408 0.34575.0652 37° C. 0.17 1.3552 0.672 0.12 1.2807 0.4724 75.0825 37° C.0.2497 1.3029 0.672 0.12 1.0746 0.6784 75.1098

FIGS. 4A-4D show the spherical aberration (in mm), astigmatism (in mm),lateral color (in mm), and distortion (in %), respectively, of themicroscope objective lens of Embodiment 2. In FIG. 4A, the label “0.8”above the ordinate indicates the maximum NA. In FIG. 4B, the astigmatismis shown for both the sagittal image surface ΔS and meridional imagesurface ΔM. In FIG. 4A, the ordinate position of the maximum NA (NA=0.8)times 0.5 and times 0.7 is labeled. In FIGS. 4B-4D, the label “11.00”above the ordinate indicates the maximum image height (in mm). In FIGS.4B and 4D, the ordinate positions of the maximum image height (11.00 mm)times 0.5 and times 0.7 are shown. In FIG. 4C, the ordinate positions ofmaximum image height (11.00) times plus 0.917 and times minus 0.917 (asmeasured vertically from the optical axis) are labeled on the ordinate,and the abscissa is labeled at −2.00 mm and +2.00 mm of lateral color.In FIGS. 4A and 4C, curves are shown for the four wavelengths listed.

FIG. 5 is a cross-sectional view of lens elements arranged along anoptical axis showing the configuration of an imaging lens that may becombined with the microscope objective lens of each embodiment of thepresent invention. Furthermore, the imaging lens shown in FIG. 5 iscommonly used with the microscope objective lens of each embodiment. Asshown in FIG. 5, the imaging lens is formed of, in order from the objectside, a cemented lens component formed of a biconvex lens element L41cemented to a negative meniscus lens element L42 having its concavesurface on the object side, and another cemented lens component formedof a biconvex lens element L43 cemented to a biconcave lens element L44.

Table 3 below lists the overall focal length ft1 (in mm) of the imaginglens shown in FIG. 5, as well as the numerical data of optical membersthat compose the imaging lens. More specifically, in the four columns ofTable 3 are listed the radius of curvature of each surface of theimaging lens in order from the object side (r24 to r29), the on-axisdistances (d24 to d28) between the optical surfaces, the refractiveindexes (nd24 to nd28) of each optical element (at the d-line wavelengthof 587.5 nm), and the Abbe numbers (νd24 to νd28) of each opticalelement (at the d-line wavelength of 587.6 nm) of the imaging lens.

TABLE 3 ft1 = 180 mm r24 = 60.4357 d24 = 8.5 nd24 = 1.497 νd24 = 81.54r25 = −67.2328 d25 = 3.8 nd25 = 1.72047 νd25 = 34.71 r26 = −640.476 d26= 10.2859 r27 = 44.0586 d27 = 8.5 nd27 = 1.72342 νd27 = 37.95 r28 =−113.8863 d28 = 4.4 nd28 = 1.6134 νd28 = 44.27 r29 = 28.0371

Table 4 below lists values of the on-axis distance d23 (in mm), asmeasured from the last surface of the objective lens to the firstsurface of the imaging lens, at two ambient temperatures, namely 21° C.(room temperature) and 37° C.

TABLE 4 at 21° C. at 37° C. Value of d23 for Embodiment 1: 80.829480.1551 Value of d23 for Embodiment 2: 79.9517 79.9517

The microscope objective lens of the present invention may be used inthe medical and biological fields where it is necessary to observe weakimages with a high signal-to-noise ratio despite the observation fieldof view being wide.

The invention being thus described, it will be obvious that the same maybe varied in many ways. For example, the two embodiments discussed indetail above are intended merely as examples and are not intended to belimiting of the invention claimed, as other construction values may beselected. Moreover, a lens component may sometimes be substituted for alens element and vice-versa. Such variations are not to be regarded as adeparture from the spirit and scope of the invention. Rather, the scopeof the invention shall be defined as set forth in the following claimsand their legal equivalents. All such modifications as would be obviousto one skilled in the art are intended to be included within the scopeof the following claims.

1-4. (canceled)
 5. A microscope objective lens comprising, in order fromthe object side: a first lens group having positive refractive powerthat includes, in order from the object side, two meniscus lenscomponents, each with its concave surface on the object side, and atleast one positive lens component; a second lens group having positiverefractive power; and a third lens group having adjacent concave lenselement surfaces that face each other and are in contact with air;wherein the second lens group satisfies the following condition:0.8≦|β2|≦1.2 where β2 is the lateral magnification of the second lensgroup when the object of the second lens group is the image formed bythe first lens group.
 6. The microscope objective lens of claim 5,wherein the following additional conditions are satisfied:7≦f0.5<NA where f is the focal length (in mm) of the microscope objectivelens, and NA is the numerical aperture on the object side of themicroscope objective lens. 7-11. (canceled)
 12. A microscope objectivelens comprising, in order from the object side: a first lens grouphaving positive refractive power that includes, in order from the objectside, a first meniscus lens component arranged nearest to the objectside and with its concave surface on the object side and in contact withair, and a second meniscus lens component with its concave surface onthe object side, and at least one positive lens component; a second lensgroup having positive refractive power; and a third lens group havingadjacent concave lens element surfaces that face each other and are incontact with air; wherein the following condition is satisfied:60<D≦120 where D is the on-axis distance (in mm) from an object underobservation to a plane where said objective lens is mounted to themicroscope body.
 13. The microscope objective lens of claim 12, whereinthe following additional conditions are satisfied:7≦f0.5<NA where f is the focal length (in mm) of the microscope objectivelens, and NA is the numerical aperture on the object side of themicroscope objective lens. 14-16. (canceled)